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4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 1
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SiC excellent electrical and thermal properties. only semiconductor material besides Si on which a thermal oxide can be grown Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 2
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Materials PropertySiSiC-4HGaN Band Gap (eV) 1.13.23.4 Critical Field 106 V/cm 0.333.5 Electron Mobility (cm2/V-sec) 14509002000 Electron Saturation Velocity (106 cm/sec) 102225 Thermal Conductivity (Watts/cm2 K) 1.551.3 Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 3
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Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 4
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STRUCTURE OF POWER MOSFET: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 5
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STRUCTURE OF 4H-SIC DMOSFET : Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 6
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STRUCTURE: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 7 The MOS channel length is defined by the p- well and n+ implants, and can range from 0.5 μm to 1.5 μm. Electron flow : n+ source - inversion layer - implanted p-well -JFET region - lightly doped n- drift region - drain.
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STRUCTURE OF Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 8 The blocking voltage of the MOSFET is determined by the doping concentration of the n- epilayer. For 1200 V devices, an epilayer with a doping concentration of 6x10 15 cm-3 and a thickness of 12 μm can be used. A thermally grown oxide layer is typically used as gate dielectric due to its repeatability and stability.
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STRUCTURE Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 9 Typically, the gate oxide is nitrided in NO or N2O to reduce MOS interface state density, which improves the transconductance of the MOSFET.
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TRANSFER CHARACTERISTICS: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 10
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OUTPUT CHARACTERISTICS: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 11
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STRUCTURE OF SiC AMLDM: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 12
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STRUCTURE: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE A thin n-channel region (accumulation-layer) below the gate oxide. Normally off device with the entire drain voltage supported by the p/n-drift region. Support high forward blocking voltages at zero gate bias with low leakage currents. 13
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STRUCTURE: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE A low resistance path for the electron current flow from the source to the drain can be achieved. This structure utilizes the buried p-well region as a shield to the influence of a high SiC bulk electric filed on the gate oxide. Removes the effect of interface quality on the channel mobility. 14
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EFECT OF ACCUMULATION LAYER THICKNESS ON OPERATING VOLTAGE AND SPECIFIC ON RESISTANCE: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 15
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TRANSFER CHARACTERISTICS: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 16
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OUTPUT CHARACTERISTICS: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 17
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OFF STATE CHARCATERISTICS: Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 18
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Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE THANK YOU 19
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